Space and Time Invariance (Classical Wave Equation)

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SUMMARY

The discussion focuses on the space and time invariance of the classical wave equation, specifically the equations \(\frac{\partial^{2}y}{\partial t^{2}} = v^{2} \cdot \frac{\partial^{2}y}{\partial x^{2}}\) and \(\frac{\partial y}{\partial t} = -v \cdot \frac{\partial y}{\partial x}\). The first equation is confirmed to be space and time invariant, while the second is not. Andrew suggests testing the simple wave function \(y(x,t) = \sin(x + vt)\) to illustrate the differences in invariance.

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  • Understanding of partial differential equations
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  • Knowledge of the concepts of space and time invariance
  • Basic calculus, particularly differentiation
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mess1n
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Hey, I've come across a part in my notes which I can't figure out. Essentially it says:

[tex]\frac{\partial^{2}y}{\partial t^{2}}[/tex] = v[tex]^{2}[/tex] . [tex]\frac{\partial^{2}y}{\partial x^{2}}[/tex] is space and time invariant.

Whereas:

[tex]\frac{\partial y}{\partial t}[/tex] = -v . [tex]\frac{\partial y}{\partial x}[/tex] is not.

Why is this the case?

Cheers,
Andrew
 
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Try putting a simple wave like y(x,t) = sin(x+vt) into both equations and see what happens.

Guessing at equations is a standard way for physicists to explore a problem.
 

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